Left- and right-handed trigonal Se and Te enantiomers exhibit opposite signs in the σ_yx^{S_y} and σ_yx^{L_y} components of spin and orbital Hall conductivities due to mirror symmetry between their space groups.
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4 Pith papers cite this work. Polarity classification is still indexing.
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Pith papers citing it
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2026 4representative citing papers
Surface fRG extension shows d-wave superconductivity from the 2D Hubbard model persists across most interlayer couplings but splits into two regimes separated by a narrow region of incommensurate spin-density-wave and spin-bond order at intermediate couplings.
d1T-phase monolayer MoS2 is predicted to be a ferroelectric higher-order topological insulator whose orbital Hall conductivity sign is switched by polarization direction.
Zn substitution stabilizes ferromagnetism in EuMn2Sb2 and induces Weyl nodes near the Fermi level through broken time-reversal and inversion symmetries.
citing papers explorer
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Probing the Chirality of Trigonal Selenium and Tellurium by Spin and Orbital Hall Effects
Left- and right-handed trigonal Se and Te enantiomers exhibit opposite signs in the σ_yx^{S_y} and σ_yx^{L_y} components of spin and orbital Hall conductivities due to mirror symmetry between their space groups.
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Surface Functional Renormalization Group for Layered Quantum Materials
Surface fRG extension shows d-wave superconductivity from the 2D Hubbard model persists across most interlayer couplings but splits into two regimes separated by a narrow region of incommensurate spin-density-wave and spin-bond order at intermediate couplings.
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Ferroelectric polarization controlled orbital Hall conductivity in a higher-order topological insulator: \textit{d1T}-phase monolayer MoS$_2$
d1T-phase monolayer MoS2 is predicted to be a ferroelectric higher-order topological insulator whose orbital Hall conductivity sign is switched by polarization direction.
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Broken Symmetry-driven Weyl Semimetal Phase in Zn-Substituted EuMn$_2$Sb$_2$
Zn substitution stabilizes ferromagnetism in EuMn2Sb2 and induces Weyl nodes near the Fermi level through broken time-reversal and inversion symmetries.